Paper-based microfluidics are microfluidic devices that consist of a series of hydrophilic cellulose or nitrocellulose fibers that transport fluid from an inlet through the porous medium to a desired outlet or region of the device, by means of capillary action. This technology builds on the conventional lateral flow test which is capable of detecting many infectious agents and chemical contaminants. The main advantage of this is that it is largely a passively controlled device unlike more complex microfluidic devices. Development of paper-based microfluidic devices began in the early 21st century to meet a need for inexpensive and portable medical diagnostic systems.
Architecture Paper-based microfluidic devices feature the following regions:
Inlet: a substrate (typically cellulose) where liquids are dispensed manually. Channels: hydrophilic sub-millimeter networks that guide liquid throughout a device. Flow amplifiers: regions of varying geometry where the flow velocity is modified to impart a steady state flow of controllable velocity Flow resistors: a capillary element used to impart a reduced flow velocity in order to control the residence time of a fluid in a microfluidic device Barriers: hydrophobic regions that prevent fluid from leaving the channel. Outlets: location where a chemical or biochemical reaction takes place.
Flow The movement of fluid through a porous medium such as paper is governed by permeability (earth sciences), geometry and evaporation effects. Collectively these factors results in evaporation limited capillary penetration that can be tuned by controlling porosity and device geometry. Paper is a porous medium in which fluid is transported primarily by wicking and evaporation. The capillary flow during wetting can be approximated by Washburn's equation, which is derived from Jurin's law and the Hagen–Poiseuille equation. The average velocity of fluid flow is generalized as, v = γ cos θ 4 η 1 L {\displaystyle v={\frac {\gamma \cos \theta }{4\eta }}{\frac {1}{L}}} where γ {\displaystyle \gamma } is the surface tension, θ {\displaystyle \theta } the contact angle, η {\displaystyle \eta } is the viscosity, and L {\displaystyle L} is the distance traveled by the liquid. More extensive models account for paper tortuosity, pore radius, and paper deformation. Once the medium is fully wetted, subsequent flow is laminar and follows Darcy's law. The average velocity of fluid flow is generalized as, v = − K η ▽ P {\displaystyle v=-{\frac {K}{\eta }}\triangledown P} where K {\displaystyle K} is the medium permeability and ▽ P {\displaystyle \triangledown P} is the pressure gradient. One consequence of laminar flow is that mixing is difficult and based solely on diffusion, which is slower in porous systems.
Manufacturing Paper-based microfluidic devices can be manufactured based on the dimensions, i.e. 2D and 3D. To fabricate 2D paper-based microfluidics, variations of methods, such as wax printing, inkjet printing, photolithography, flexographic printing, plasma treatment, laser treatment, etching (microfabrication), screen printing, digital light processing (DLP) 3-D printer, and wax screening, have been employed. Further lamination of multiple paper microfluidics creates pseudo-3D microfluidics that could provide an additional dimension of the fluidic network and increase the complexity. Each technique aims to create hydrophobic physical barriers on hydrophilic paper that passively transport aqueous solutions. Biological and chemical reagents must then be deposited selectively along the device by either dipping the substrate into a reagent solution or locally spotting a reagent onto the substrate.
Wax printing Wax printing uses a simple printer to pattern wax on paper in a desired design. The wax is then melted with a hotplate to create channels. This technique is fast and low cost, but has relatively low resolution due to the isotropy of the melted wax.
Inkjet printing Inkjet printing requires coating paper in a hydrophobic polymer, and then selectively placing an ink that etches the polymer to reveal paper. This technique is low cost with high resolution, but is limited by the speed of placing one ink droplet at a time.
Photolithography Photolithographic techniques are similar to inkjet printing, using a photomask to selectively etch a photoresist polymer. This technique has high resolution and is quick, but has high equipment and material costs.
DLP printing This technique utilizes a DLP printing technique in which photo-curable resin polymers are exposed to lights to form hydrophobic boundaries of open microchannels in a porous paper. If the effects of evaporation are of concern in the specific application then two additional layers of the curable resin can be used on the top and bottom of the channel. Excess uncured resin is then cleaned off using ethanol. This technique has relatively low equipment costs and utilizes readily available materials making it a promising candidate for mass production of point of care diagnostic devices.
Plasma processing In this technique, paper is first rendered hydrophobic using a hydrophobizing agent such as AKD or fluorocarbon plasma polymerization, and then O2 plasma etching with a mask is used to create hydrophilic patterns in the paper. One benefit of plasma based processes is that the complex designs and functionalities such as fully and semi-enclsoed channels, on-off flow switches, and fluid flow control channels can be incorporated relatively easily. However, cost of production is relatively higher than other fabrication methods.
Analytical applications
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